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This course contains solution of non linear equations and linear system of equations, approximation of eigen values, interpolation and polynomial approximation, numerical differentiation, integration, numerical solution of ordinary differential equations. This lecture includes: Jacobi, Method, Orthogonal, Eigenvectors, Symmetric, Matrix, Theory, Diagonal, Transformations, Construct, Row
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Definition An n x n matrix [ A ] is said to be orthogonal if
1
i.e.[ ] [ ]
T T
In order to compute all the eigen values and the corresponding eigenvectors of a real symmetric matrix, Jacobi’s method is highly recommended. It is based on an important property from matrix theory, which states that, if [ A ] is an n x n real symmetric matrix, its eigen values are real, and there exists an orthogonal matrix [ S ] such that the diagonal matrix D is [ S −^1 ][ A ][ S ]
This digitalization can be carried out by applying a series of orthogonal transformations S 1 (^) , S 2 ,..., Sn ,
diagonal elements of A. We construct an orthogonal matrix S 1 defined as
sin , sin , cos , cos
ij ji ii jj
s s s s
While each of the remaining off-diagonal elements are zero, the remaining diagonal elements are assumed to be unity. Thus, we construct S 1 as under
1
i-th column -th column
0 0 cos sin 0 i-th row
0 0 sin cos 0 -th row
0 0 0 0 1
j
j
and elsewhere it is identical with a unit matrix. Now, we compute D 1 (^) = S 1 − 1 AS 1 (^) = S 1 T AS 1 Since S1 is an orthogonal matrix, such that .After the transformation, the elements at the position (i , j), (j , i) get annihilated, that is dij and dji reduce to zero, which is seen as follows:
2 2 2 2
cos sin cos sin sin cos sin cos cos sin cos sin ( ) sin cos cos 2 ( ) sin cos cos 2 sin cos 2 sin cos
ii ij ji jj ii ij ij jj ii jj jj ii ij ji ii ij ii jj ij
d d d d a a a a a a a a a a a a a a a a
θ θ θ θ θ θ θ θ θ θ θ θ θ θ θ θ θ θ θ θ θ θ
cos 2 sin 2 0 2
jj ii ij
That is if
tan 2 2 ij ii jj
a a a
and dji reduces to zero.However, though it creates a new pair of zeros, it also introduces non-zero contributions at formerly zero positions. Also, the above equation gives four values of , but to get the least possible rotation, we choose